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Pump Summit 2014, 2 – 3 December 2014, Düsseldorf
Fast Centrifugal Oil Pump Design and
Automated Evaluation by 3D-CFD
Eduard Moser, Ralph-Peter Mueller, Anne Schubert, Dr. Oliver Velde
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
CFturbo® Software & Engineering GmbH
Engineering CAD & Prototyping
• Turbomachinery Conceptual Design
• CFD/FEA Simulation
• Optimization
• 3D-CAD Modeling
• Prototyping
• Testing, Validation
CFturbo® Software
• Turbomachinery Design Software
• Automated Workflows
CFturbo® - The Turbomachinery Design Company
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
CFturbo® - Input and Output Data
CFturbo®
Fundamental equationsEuler-eq. of Turbomachinery,
Continuity equation, Momentum equation, …
Empirical functionsPublic knowledge,
Proprietory Know-How Existing geometry-elements, imported
Reference geometry –elements, from CFturboDefine operating point
Q, Dp, speed, Fluid propertiesInlet conditions New and / or
modifiedcomponents
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Turbomachinery Development Process using CFturbo®
ConceptualDesign
CFturbo®
MeshingANSA, AutoGrid, ICEM, Pointwise, TurboGrid, …
3D-CADAutoCAD, Creo, Inventor,
NX, SolidWorks, …
ProductionRe-computation/optimizationinteractively or automated
CFD/FEA SimulationSTAR CCM+, ANSYS-CFX,FINE/Turbo, PumpLinx, …
ExperimentsPrototyping,
Validation
Design Simulation & Validation Product
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
CFturbo® - Interfaces to selected 3D-CFD-Codes
CFturbo®
ANSYS ANSYS-CFX
ESI/Open CFD OpenFOAM
NUMECA FINE/Turbo
PumpLinx
STAR CCM+
ICEM, TurboGrid
Snappy Hex Mesh
AutoGrid, HexPress
Simerics
CD-adapco
Seamless interfaces for automated workflows and optimization
Conceptual Design Meshing Simulation
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Conceptual Design of the Pump Stage
DESIGN POINT
Volume flow Q 2,75 m³/hPresssure rise DP 1,50 barSpeed n 6.000 rpmFluid Density r20 936 kg/m³
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Automated Meshing
Direct Interface in CFturbo
Using PumpLinx® to createcarthesian binary tree mesh
Approx. 2,0 mio. nodes
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Steady State (MFR) and Transient Simulation
Hardware: Modern desktop workstation, 8 cores
Computational time - Steady State (MFR) 20 … 30 min. /operating point- Transient 3 hours/operating point- Batch mode runs
Steady State (MFR) Transient
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Design & Simulation Process
CAE-engineering process to design and simulate the oil pump, 8 model variations, delivery time less than one week
Design point defintion
Volume flow Q 2,75 m³/hPresssure rise DP 1,50 barSpeed n 6.000 rpmFluid Density r20 936 kg/m³
Modified fluid data for simulation (oil)
Density (20°) r20 936 kg/m³Density (70°) r70 890 kg/m³Viscosity (20°) n20 0.009 Pa sViscosity (70°) n70 0.004 Pa s
8 Designs 8 Performance curves 1 Prototype built
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Fluid PropertiesDensity= f (Temperature)
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
-50 0 50 100 150 200
r [
kg/m
³]
T [°C]
Oil (SYLTHERM 800) WATER
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Fluid PropertiesDynamic Viscosity = f (Temperature)
0
10
20
30
40
50
60
70
-50 0 50 100 150 200
h[m
Pas
]
T [°C]
Oil (SYLTHERM 800) WATER
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
0
25000
50000
75000
100000
125000
150000
175000
200000
0 1 2 3 4 5
Dp
tot,
Stag
e[P
a]
Q [m³/h]
Oil T-25 Oil T0 Oil T25 Oil T70 Oil T100 Water T25
Simulation Results – MFR
Pump Performance Curves = f (Volume Flow, Temperature)
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Simulation Results – MFR
Hydraulic Efficiency = f (Volume Flow, Temperature)
0,00
0,10
0,20
0,30
0,40
0,50
0,60
0,70
0 1 2 3 4 5
h[-
]
Q [m³/h]
Oil T-25 Oil T0 Oil T25 Oil T70 Oil T100 Water T25
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
0,00
0,10
0,20
0,30
0,40
0,50
0,60
0,70
20000
40000
60000
80000
100000
120000
140000
160000
180000
0 0,005 0,01 0,015 0,02 0,025 0,03 0,035 0,04
h[-
]
Dp
tot,
Stag
e[P
a]
Dynamic viscosity h [Pas]
Q=2,75m³/h
Dptot,Stage h [-]
Simulation Results – MFR
Hydraulic Efficiency, Total Pressure Difference = f (Dynamic Viscosity)
0,00
0,10
0,20
0,30
0,40
0,50
0,60
0,70
20000
40000
60000
80000
100000
120000
140000
160000
180000
-50 0 50 100 150 200 250
h[-
]
Dp
tot,
Stag
e
T [°C]
Q=2,75m³/h
Dptot,Stage h [-]
Hydraulic Efficiency, Total Pressure Difference = f (Oil Temperature)
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Simulation Results – MFR
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Static Pressure and Velocity Magnitude @ [T=70°C, Q=2.75 m³/h)
Results – transient flow
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Results – transient flow
0
20000
40000
60000
80000
100000
120000
140000
160000
180000
0 1 2 3 4 5
Dp
tot,
Stag
e[P
a]
Q [m³/h]
T-25T-25 transT0T0 transT25T25 transT70T70 transT100
Performance Map Simulation - Transient vs. Steady State (MFR)
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Results – transient flow
Hydraulic Efficiency Simulation - Transient vs. Steady State (MFR)
0,00
0,10
0,20
0,30
0,40
0,50
0,60
0,70
0 1 2 3 4 5
h[-
]
Q [m³/h]
ÖL
T-25 T-25 trans
T0 T0 trans
T25 T25 trans
T70 T70 trans
T100 T100 trans
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Summary - Important Issues for successful design
- Consider all details of pump geometry in early design stage, if possible
- For oil pumps the temperature dependency of fluid properties is importantto perfomance map simulation and efficiency prediction
- Density and viscosity are design relevant and should be used by empiricalcorrelations in early conceptual design phase of a project
- Transient 3D-CFD-simulations should be used for a more accurateperfomance prediction and design decisions, compared to MFR
PUMP SUMMIT 2014, 2 – 3 DECEMBER 2014, DÜSSELDORF
Summary
The classical design theory of centrifugal pumps uses a large empirical data base for parameters that cannot beeasily described using a pure theoretical approach. This empirical knowledge has been achieved on the basis ofcentrifugal pumps meant to convey water and has been proven to be reliable over the last decades.
On the other hand due to the fact that the automotive sector is under strong pressure to develop more efficient carsthe hybridization of the complete drive concept is proceeding significantly. In this context it is more and moreinteresting to use centrifugal pumps for the transport of oil in the engine or gear box. Here the higher viscosity of oilagainst water is an issue that weakens the so far used set of empirical co-relations in the design process, because itcannot easily transformed into a comprehensive and reliable empirical knowledge basis for the design of centrifugaloil pumps.
It is state of the art that in the design process of centrifugal pumps simulation techniques are widely used prior a realhardware test. This saves a lot of time and money as the first prototype is very close to a hydraulically good machine.By trend the design of centrifugal oil pumps is a more lengthy process compared to that of water pumps as theempirical data base is weaker and more design cycles are necessary. Therefore a highly automated and robustworkflow is desired that comprehends both the CAD-design of the pump as well as the test of the current designusing modern simulation techniques.
In this paper a method has been presented that uses empirical correlations to adapt water pump design rules to oilpumps and establishes and fully automated CFD workflow for virtual testing. It allows an almost immediate responsefrom the simulation environment once the design of the hydraulic components has been finished. Using thisapproach design and test are not any longer separate processes but are seamlessly connected. One gets a straightanswer on every design parameter change and can go through the design process very intuitively and is herewith notreliant on an accurate empirical data basis. In future more and more correlations can be computed for oil and otherfluids by the use of cloud computing. New knowledge will become available for conceptual design of oil pumps too.